TM dual mode dielectric resonator and filter

Abstract: In a TM dual mode dielectric resonator apparatus, a cross-shaped TM dual mode dielectric resonator is provided in an electrically conductive case, wherein the TM dual mode dielectric resonator comprises first and second dielectric resonators integrally formed so as to be perpendicular to each other, and coupling grooves for coupling an operation mode of the first dielectric resonator with an operation mode of the second dielectric resonator are formed in the TM dual mode dielectric resonator. Cross-sectional areas or sizes such as thickness, widths or the like, of the first and second dielectric resonators are set so as to be different from each other. Alternatively, a hole for adjusting the resonance frequency is formed at an end of one of the first and second dielectric resonators so as to penetrate the same.

Description: The present invention relates to a dielectric resonator apparatus and a high-frequency band-pass filter apparatus utilizing the dielectric resonator apparatuses, and in particular, to a TM dual mode dielectric resonator apparatus and a high-frequency band-pass filter apparatus utilizing the TM dual mode dielectric resonator apparatuses. Fig. 9 is a partially broken perspective view of a conventional high frequency four-stage band-pass filter apparatus 51, which comprises two single mode dielectric resonator 52 and 53 and one TM dual mode dielectric resonator 54 which are provided within a metal case 55. Referring to Fig. 9, each of the single mode dielectric resonators 52 and 53 is constituted by providing a TM mode dielectric resonator 57 provided within an electrically conductive case 56 which functions as a waveguide. Further, the TM dual mode dielectric resonator 54 is constituted by providing within an electrically conductive case 61, a TM dual mode dielectric resonator 60 integrally formed in a shape of a cross of two TM mode dielectric resonators 58 and 59 so that the TM mode dielectric resonators 58 and 59 are perpendicular to each other, and the TM dual mode dielectric resonator 60 has coupling grooves 70 for coupling an operation mode of the even mode with that of the odd mode. The TM dual mode dielectric resonator 54 is disclosed in, for example, the Japanese Patent Laid-open Publication No. 61-121502. In the conventional band-pass filter apparatus 51, a Qe coupling loop 63, which is provided on the side of the inner surface of a coaxial input and output connector 62 provided on one end surface of a metal case 64 and which is electrically connected to the coaxial input and output connector 62, is magnetically coupled with the TM mode dielectric resonator 57 of the single mode dielectric resonator apparatus 52 of the first stage, which is magnetically coupled with the TM dual mode dielectric resonator 60. Further, the TM dual mode dielectric resonator 60 is magnetically coupled with the TM mode dielectric resonator 57 of the single mode dielectric resonator apparatus 53 of the final stage, which is magnetically coupled with another Qe coupling loop 63 electrically connected to another coaxial input and output connector 62. This results in the four-stage band-pass filter apparatus 51. In the case of using the two TM dual mode dielectric resonator, since the two TM mode dielectric resonators are integrally formed in a form of a cross, it is considered that the size of the filter apparatus can be reduced as compared with such a case that there are provided two single mode dielectric resonators. Therefore, in the above-mentioned four-stage band-pass filter apparatus, if the two TM dual mode dielectric resonators can be utilized, it is expected that the size of the band-pass filter apparatus can be further reduced. However, in the conventional TM dual mode dielectric resonator, the TM mode two dielectric resonators thereof have the same resonance frequency in such a state that they are not installed within the filter apparatus. Therefore, in the case where the TM dual mode dielectric resonator is installed within the above-mentioned filter apparatus, when the TM dual mode dielectric resonator is provided so as to be coupled with the Qe coupling loop, the resonance frequency of one TM mode dielectric resonator thereof magnetically coupled with the Qe coupling loop becomes different from that of another TM mode dielectric resonator thereof not coupled with the Qe coupling loop due to influence of the Qe coupling loop. When the two TM mode dielectric resonators of the TM dual mode dielectric resonator have different resonance frequencies from each other, we can not decide the coupling coefficient between the operation modes of the two rectangular-parallelepipedshaped TM mode dielectric resonators of the TM dual mode dielectric resonator based on the resonance frequency f even of the even mode and the resonance frequency f odd of the odd mode. Accordingly, in the conventional apparatuses, as shown in the filter apparatus of Fig. 9, the single mode dielectric resonators 52 and 53 are magnetically coupled with the Qe coupling loops 63. In this case, there is such a problem that the size of the conventional filter apparatus can not be further reduced. In the article: "800MHz High Power Duplexer using TM dual mode dielectric resonators" of Ishikawa et al. in 1992 IEEE MTT-S International Microwave Symposium Digest, vol. III, 1-5 June 1992, New York, pages 1617-1620, a full monoblock type TM 110 dual mode resonator in the 800MHz band and a duplexer using a plurality of these dielectric resonators is described. The dual mode resonator is formed in a cross-shaped form of a dielectric material and by means of a dielectric rod, the resonance frequency is tuned. The coupling constant is controlled by the shape and volume of removed dielectric material. Starting from this prior art, it is the object underlying the present invention to provide for an improved dielectric resonator apparatus. This object is achieved by a dielectric resonator apparatus according to claim 1 and by a dielectric resonator apparatus according to claim 5. According to one preferred embodiment of the present invention, a high-frequency band-path filter apparatus is provided which comprises two dielectric resonator apparatus, each being magnetically coupled with a Qe coupling loop, wherein respective resonance frequencies of two TM mode dielectric resonators of each TM dual mode dielectric resonators can be respectively adjusted so that the respective resonance frequencies of the two TM mode dielectric resonators become equal to each other in such a state that one TM mode dielectric resonator thereof is magnetically coupled with a Qe coupling loop. Therefore, the TM dual mode dielectric resonator apparatus can be used in the stage coupling with the coupling loop. This results in reduction in the size of the high-frequency band-pass filter apparatus. These and other objects and features of the present invention will become clear from the following description taken in conjunction with the preferred embodiments thereof with reference to the accompanying drawings throughout which like parts are designated by like reference numerals, and in which: Fig. 1A is a perspective view of a TM dual mode dielectric resonator apparatus according to a first preferred embodiment of the present invention; Fig. 1B is a cross-sectional view along a line IB - IB' of Fig. 1A; Fig. 2 is a front view of a TM dual mode dielectric resonator apparatus according to a second preferred embodiment of the present invention; Fig. 3 is a partially broken perspective view of a high frequency four-stage band-pass filter apparatus according to a third preferred embodiment of the present invention; Fig. 4 is an exploded view showing the main portion of the high frequency four-stage band-pass filter apparatus shown in Fig. 3; Fig. 5A is a perspective view of a TM dual mode dielectric resonator apparatus according to a fourth preferred embodiment of the present invention; Fig. 5B is a cross-sectional view along a line VB - VB' of Fig. 5A; Fig. 6 is a graph showing a relationship between a differences between resonance frequencies of TM mode dielectric resonators of the TM dual mode dielectric resonator shown in Figs. 5A and 5B and a diameter of a hole for adjusting the resonance frequency formed in one TM mode dielectric resonator; Fig. 7 is a partially broken perspective view of a high frequency four-stage band-pass filter apparatus according to a fifth preferred embodiment of the present invention; Fig. 8 is an exploded view showing the main portion of the high frequency four-stage band-pass filter apparatus shown in Fig. 7; and Fig. 9 is a partially broken perspective view of a conventional high frequency four-stage band-pass filter apparatus. The preferred embodiments according to the present invention will be described below with reference to the attached drawings. FIRST PREFERRED EMBODIMENT Fig. 1A is a perspective view of a TM dual mode dielectric resonator apparatus 200a according to a first preferred embodiment of the present invention, and Fig. 1B is a cross-sectional view along a line IB - IB' of Fig. 1A. Referring to Fig. 1A, a dual mode dielectric resonator apparatus 200a is constituted by integrally providing a TM dual mode dielectric resonator 2 within a rectangular-cylinder-shaped electrically conductive case 1 which functions as a waveguide. The electrically conductive case 1 is constituted by a metal case, or by forming an earth electrode on surfaces of a case main body made of a dielectric ceramics material in a forming manner similar to that of the TM dual mode dielectric resonator 2 by plating the surfaces thereof with a Ag paste or the like. Further, the TM dual mode dielectric resonator 2 is integrally formed in a shape of a cross of two rectangular-cylinder-shaped TM mode dielectric resonators 3a and 3b made of a dielectric ceramics each TM mode dielectric resonator having, for example, TM 110 mode so that the TM mode dielectric resonators 3a and 3b are perpendicular to each other. In the present preferred embodiment, as shown in Fig. 1B, the respective TM mode dielectric resonators 3a and 3b are formed so that the thickness Tb in a depth direction from the front surface towards the back surface of one TM mode dielectric resonator 3b vertically installed is greater than the thickness Ta in the depth direction from the front surface towards the back surface of another TM mode dielectric resonator 3a horizontally installed. In the case 1 made of a metal material, the TM dual mode dielectric resonator 2 is electrically and mechanically coupled with the inner surfaces of the case 1 through electrically conductive layers (not shown) of Ag thick films formed both the end surfaces of the respective TM mode dielectric resonators 3a and 3b. As shown in Fig. 1A, the following electric lines of force are generated in the TM dual mode dielectric resonator 2: (a) electric lines E 1 and E 2 of force of the respective dielectric resonators 3a and 3b indicated by alternate long and short dash lines; (b) electric lines Ee of force of the even mode indicated by dotted lines; and (c) the other electric lines Eo of force of the odd mode indicated by real lines. In the top right corner and the bottom left corner of a crossing portion of the two TM mode dielectric resonators 3a and 3b (referred to as a crossing portion hereinafter) formed in a shape of the cross of the TM dual mode dielectric resonator 2, coupling grooves 4 for coupling an operation mode or a resonance oscillation of the TM mode dielectric resonator 3a with that of the TM mode dielectric resonator 3b are formed so as to extend from the front surface of the crossing portion towards the back surface thereof and so as to have depths in a diagonal direction of the crossing portion, respectively. The coupling grooves 4 are formed in order to cut the electric lines Ee of force of the even mode. The coupling coefficient between the two TM mode dielectric resonators 3a and 3b can be adjusted by adjusting the depths and/or widths of the coupling grooves 4. The coupling grooves 4 may be formed in the top left corner and the bottom right corner of the crossing portion of the two TM mode dielectric resonators 3a and 3b so as to cut the electric lines Eo of force of the odd mode. In the present preferred embodiment, since the thickness Tb of the TM mode dielectric resonator 3b vertically installed is greater than the thickness Ta of the TM mode dielectric resonator 3a horizontally installed, the effective dielectric constant of the TM mode dielectric resonator 3b becomes greater than that of the TM mode dielectric resonator 3a. In this case, the resonance frequency of the TM mode dielectric resonator 3b is lower than that of the TM mode dielectric resonator 3a. In the case of only the TM dual mode dielectric resonator apparatus 200a which is formed so that the respective thickness of the TM mode dielectric resonators 3a and 3b are different from each other, there is caused a difference between the resonance frequencies of the TM mode dielectric resonators 3a and 3b. The present preferred embodiment of the present invention utilizes this phenomenon. Therefore, the difference between the thicknesses of the respective TM mode dielectric resonators 3a and 3b can correct the difference between the resonance frequencies of the TM mode dielectric resonators 3a and 3b, which are formed so as to be crossed to be perpendicular to each other, so as to be zero. Further, when one TM mode dielectric resonator, for example, 3b is magnetically coupled with a Qe coupling loop, the resonance frequency of the TM mode dielectric resonator 3b is shifted from the original resonance frequency thereof so as to be higher than the original resonance frequency thereof due to the magnetic coupling. In this case, this shift in the resonance frequency of the TM mode dielectric frequency 3b can be corrected so as to be zero, by adjusting the thickness Tb of the TM mode dielectric resonator 3b so as to be greater than the thickness Ta of the TM mode dielectric resonator 3a. In such a state that one TM mode dielectric resonator 3b is coupled with a Qe coupling loop, the respective resonance frequencies of the TM mode dielectric resonators 3a and 3b can be set to be equal to each other through the above-mentioned adjustment. When the depths or widths of the coupling grooves 4 are changed, the coupling coefficient between the TM mode dielectric resonators 3a and 3b can be adjusted. In this case, when the respective resonance frequencies of the TM mode dielectric resonators 3a and 3b are adjusted so as to be equal to each other, the coupling coefficient can be decided or calculated based on the resonance frequency f even of the even mode and the resonance frequency f odd of the odd mode. The respective TM mode dielectric resonator 2 may be formed so that the thickness Tb of the TM mode dielectric resonator 3b is smaller than the thickness Ta of the TM mode dielectric resonator 3a. SECOND PREFERRED EMBODIMENT Fig. 2 is a front view of a TM dual mode dielectric resonator apparatus 200b according to a second preferred embodiment of the present invention; Referring to Fig. 2, in the TM dual mode dielectric resonator apparatus 200b, the TM dual mode dielectric resonator 2 is constituted by a pair of TM mode dielectric resonators 3a and 3b which are formed so that the width Wb on the front and back surfaces of the TM mode dielectric resonator 3b vertically installed is greater than the width Wa on the front and back surfaces of the TM mode dielectric resonator 3a. This results in that the effective dielectric constant of the TM mode dielectric resonator 3b vertically installed becomes greater than that of the TM mode dielectric resonator 3a horizontally installed. As a result, the resonance frequency of the TM mode dielectric resonator 3b becomes lower than that of the TM mode dielectric resonator 3a. Further, the respective resonance frequencies of the TM mode dielectric resonators 3a and 3b may be different from each other by setting both the thicknesses in the depth direction and the widths of the two TM mode dielectric resonators 3a and 3b so that the thicknesses thereof are different from each other and the widths thereof are different from each other. Furthermore, in the case of circular-cylindrical TM mode dielectric resonators 3a and 3b, the diameters thereof may be different from each other. In other words, the cross-sectional areas of the two TM mode dielectric resonators 3a and 3b may be different from each other. In this case, the same advantageous effects can be obtained as that of the above-mentioned case. Even though each of the two TM mode dielectric resonators 3a and 3b has an elongated slot or a space therein and they have the same depths and the same widths, the cross-sectional areas of the two TM mode dielectric resonators 3a and 3b may be different from each other. In this case, the same advantageous effects can be obtained as that of the above-mentioned case. THIRD PREFERRED EMBODIMENT Fig. 3 is a partially broken perspective view of a high frequency four-stage band-pass filter apparatus 210 according to a third preferred embodiment of the present invention, and Fig. 4 is an exploded view showing the main portion of the high frequency four-stage band-pass filter apparatus 210 shown in Fig. 3. Referring to Fig. 3, within a rectangular-cylindrical metal case 11, two TM dual mode dielectric resonator apparatuses 200-1 and 200-2 having a structure shown in Figs. 1A and 1B or 2 are provided so as to be apart and so that the front and back surfaces of the crossing portions thereof are parallel to each other. As shown in Fig. 4, the TM mode dielectric resonator 3b vertically installed of the TM dual mode dielectric resonator apparatus 200-1 is magnetically coupled with a Qe coupling loop 13a electrically connected to a coaxial input and output connector 12 provided in the case 11, whereas the TM mode dielectric resonator 3b vertically installed of the TM dual mode dielectric resonator apparatus 200-2 is magnetically coupled with a Qe coupling loop 13b electrically connected to another coaxial input and output connector 12 provided in the case 11. Between the two TM dual mode dielectric resonator apparatuses 200-1 and 200-2, there is provided a partition plate 15 of a metal material having an electrode pattern formed thereon, and having a plurality of strip-shaped slits 14 which are parallel to each other and to the longitudinal directions of the TM mode dielectric resonators 3b and 3b of the TM dual mode dielectric resonators 200-1 and 200-2 and which are formed vertically. Then the TM mode dielectric resonator 3a of the TM dual mode dielectric resonators 200-1 is magnetically coupled with the TM mode dielectric resonator 3a of the TM dual mode dielectric resonators 200-2 through the slits 14 of the partition plate 15. In the preferred embodiment, the TM dual mode dielectric resonator apparatuses 200-1 and 200-2 are provided at the stages coupling with the Qe coupling loops 13a and 13b, and the resonance frequencies of the TM mode dielectric resonators 3b and 3b coupled with the Qe coupling loops 13a and 13b are influenced. In the high-frequency band-pass filter apparatus 210, the respective resonance frequencies of the TM mode dielectric resonator 3a not coupled with the Qe coupling loop 13a or 13b and the TM mode dielectric resonator 3b coupled with the Qe coupling loop 13a or 13b can be adjusted so as to be the same as each other by adjusting the thickness of each of the TM mode dielectric resonators 3b and 3b. Therefore, the coupling coefficient can be adjusted to a desirable value based on the resonance frequency f even of the even mode and the resonance frequency f odd of the odd mode. Accordingly, the TM dual mode dielectric resonator apparatus can be provided at the stage coupling with the Qe coupling loop 13a or 13b. This results in reduction in the size and the weight of the high-frequency band-pass filter apparatus 210. FOURTH PREFERRED EMBODIMENT Fig. 5A is a perspective view of a TM dual mode dielectric resonator apparatus 201a according to a fourth preferred embodiment of the present invention, and Fig. 5B is a cross-sectional view along a line VB - VB' of Fig. 5A. Referring to Fig. 5A, a dual mode dielectric resonator apparatus 201a is constituted by integrally providing a TM dual mode dielectric resonator 102 within a rectangular-cylinder-shaped electrically conductive case 101 which functions as a waveguide. The electrically conductive case 101 is constituted by a metal case, or by forming an earth electrode on surfaces of a case main body made of a dielectric ceramics material in a forming manner similar to that of the TM dual mode dielectric resonator 102 by plating the surfaces thereof with a Ag paste or the like. Further, the TM dual mode dielectric resonator 102 is integrally formed in a shape of a cross of two rectangular-cylinder-shaped TM mode dielectric resonators 103a and 103b made of a dielectric ceramics each TM mode dielectric resonator having, for example, TM 110 mode so that the TM mode dielectric resonators 103a and 103b are perpendicular to each other. It is to be noted that the width and depth of the TM mode dielectric resonator 103a is the same as those of the TM mode dielectric resonator 103b. In the case 101 made of a metal material, the TM dual mode dielectric resonator 102 is electrically and mechanically coupled with the inner surfaces of the case 101 through electrically conductive layers (not shown) of Ag thick films formed both the end surfaces of the respective TM mode dielectric resonators 103a and 103b. As shown in Fig. 5A, the following electric lines of force are generated in the TM dual mode dielectric resonator 102: (a) electric lines E 1 and E 2 of force of the respective dielectric resonators 103a and 103b indicated by alternate long and short dash lines; (b) electric lines Ee of force of the even mode indicated by dotted lines; and (c) the other electric lines Eo of force of the odd mode indicated by real lines. In the top right corner and the bottom left corner of a crossing portion of the two TM mode dielectric resonators 103a and 103b (referred to as a crossing portion hereinafter) formed in a shape of the cross of the TM dual mode dielectric resonator 102, coupling grooves 104 for coupling an operation mode or a resonance oscillation of the TM mode dielectric resonator 103a with that of the TM mode dielectric resonator 103b are formed so as to extend from the front surface of the crossing portion towards the back surface thereof and so as to have depths in a diagonal direction of the crossing portion, respectively. The coupling grooves 104 are formed in order to cut the electric lines Ee of force of the even mode. The coupling coefficient between the two TM mode dielectric resonators 103a and 103b can be adjusted by adjusting the depths and/or widths of the coupling grooves 104. In the present preferred embodiment, as shown in Fig. 5B, at the end of one TM mode dielectric resonator 103b among the two TM mode dielectric resonators 103a and 103b integrally formed so as to be perpendicular to each other, a circular-cylindrical hole 105 for adjusting the resonance frequency is formed so as to penetrate the end of the TM mode dielectric resonator 103b from the right side surface thereof to the left side surface thereof. In such a state that there is formed no hole 105, the resonance frequencies of the TM mode dielectric resonators 103a and 103b are the same as each other. However, when the hole 105 is formed in the TM mode dielectric resonator 103b, or when the diameter or size of the hole 105 is made greater, the effective dielectric constant of the TM mode dielectric resonator 103b becomes smaller than that of the TM mode dielectric resonator 103a. Then the resonance frequency of the TM mode dielectric resonator 103b becomes higher than that of the TM mode dielectric resonator 103a. Fig. 6 shows a relationship between a differences between resonance frequencies of the TM mode dielectric resonators 103a and 103b of the TM dual mode dielectric resonator 102 shown in Figs. 5A and 5B and a diameter of the hole 105 for adjusting the resonance frequency. As is apparent from Fig. 6, as the diameter or size of the hole 105 is greater, the difference between the resonance frequencies of the TM mode dielectric resonators 103a and 103b is greater. In the case of only the TM dual mode dielectric resonator apparatus 201a wherein there is formed the hole 105 for adjusting the resonance frequency, there is caused a difference between the resonance frequencies of the TM mode dielectric resonators 103a and 103b. The present preferred embodiment of the present invention utilizes this phenomenon. Therefore, forming the hole 105 for adjusting the resonance frequency can correct the difference between the resonance frequencies of the TM mode dielectric resonators 103a and 103b, which are formed so as to be crossed to be perpendicular to each other, so as to be zero. Further, when one TM mode dielectric resonator, for example, 103a is magnetically coupled with a Qe coupling loop, the resonance frequency of the TM mode dielectric resonator 103a is shifted from the original resonance frequency thereof so as to be higher than the original resonance frequency thereof through the magnetic coupling. In this case, the resonance frequency of the TM mode dielectric resonator 103b can be made higher than the original resonance frequency by forming the hole 105 for adjusting the resonance frequency in another TM mode dielectric resonator 103b. Further, by adjusting the diameter or size of the hole 105 for adjusting the resonance frequency, for example, in such a state that one TM mode dielectric resonator 103b is magnetically coupled with a Qe coupling loop, the respective resonance frequencies of the TM mode dielectric resonators 103a and 103b can be set to be equal to each other. When the depths or widths of the coupling grooves 104 are changed, the coupling coefficient between the TM mode dielectric resonators 103a and 103b can be adjusted. In this case, when the respective resonance frequencies of the TM mode dielectric resonators 103a and 103b are adjusted so as to be equal to each other, the coupling coefficient can be decided or calculated based on the resonance frequency f even of the even mode and the resonance frequency f odd of the odd mode. In the preferred embodiment, the hole 105 may be formed at the end of the TM mode dielectric resonator 103a. FIFTH PREFERRED EMBODIMENT Fig. 7 is a partially broken perspective view of a high frequency four-stage band-pass filter apparatus 211 according to a fifth preferred embodiment of the present invention, and Fig. 8 is an exploded view showing the main portion of the high frequency four-stage band-pass filter apparatus shown in Fig. 7. Referring to Fig. 7, within a rectangular-cylindrical metal case 111, two TM dual mode dielectric resonator apparatuses 201-1 and 201-2 each having a structure shown in Figs. 5A and 5B are provided so as to be apart and so that the front and back surfaces of the crossing portions thereof are parallel to each other. As shown in Fig. 8, the TM mode dielectric resonator 103a horizontally installed of the TM dual mode dielectric resonator apparatus 201-1 is magnetically coupled with a Qe coupling loop 113a electrically connected to a coaxial input and output connector 112 provided in the case 111, whereas the TM mode dielectric resonator 103a horizontally installed of the TM dual mode dielectric resonator apparatus 201-2 is magnetically coupled with a Qe coupling loop 113b electrically connected to another coaxial input and output connector 112 provided in the case 111. Between the two TM dual mode dielectric resonator apparatuses 201-1 and 201-2, there is provided a partition plate 115 of a metal material having an electrode pattern formed thereon, and having a plurality of strip-shaped slits 114 which are parallel to each other and to the longitudinal directions of the TM mode dielectric resonators 103a and 103a of the TM dual mode dielectric resonators 201-1 and 201-2 and which are formed horizontally. Then the TM mode dielectric resonator 103b of the TM dual mode dielectric resonators 201-1 is magnetically coupled with the TM mode dielectric resonator 103b of the TM dual mode dielectric resonators 201-2 through the slits 114 of the partition plate 115. In the preferred embodiment, the TM dual mode dielectric resonator apparatuses 201-1 and 201-2 are provided at the stages coupling with the Qe coupling loops 113a and 113b, and the resonance frequencies of the TM mode dielectric resonators 103a and 103a coupled with the Qe coupling loops 113a and 113b are influenced. In the high-frequency band-pass filter apparatus 211, the respective resonance frequencies of the TM mode dielectric resonator 103b not coupled with the Qe coupling loop 113a or 113b and the TM mode dielectric resonator 103a coupled with the Qe coupling loop 113a or 113b can be adjusted so as to be the same as each other by adjusting the diameter or size of the holes 105 and 105 for adjusting the resonance frequency which is formed in the TM mode dielectric resonators 103b and 103b. Therefore, the coupling coefficient can be adjusted to a desirable value based on the resonance frequency f even of the even mode and the resonance frequency f odd of the odd mode. Accordingly, the TM dual mode dielectric resonator apparatus can be provided at the stage coupling with the Qe coupling loop 113a or 113b. This results in reduction in the size and the weight of the high-frequency band-pass filter apparatus 211. Furthermore, the shift of the resonance frequency between the TM mode dielectric resonators 103a and 103b due to coupling between the TM mode dielectric resonators 103a and 103b which are formed so as to be perpendicular to each other can be corrected to be zero in a similar manner. According to the TM dual mode dielectric resonator apparatus of the preferred embodiments of the present invention, the respective resonance frequencies of the two TM mode dielectric resonators thereof can be adjusted so that the respective resonance frequencies of the two TM mode dielectric resonators become equal to each other in such a state that one TM mode dielectric resonator thereof is magnetically coupled with a Qe coupling loop. Therefore, the TM dual mode dielectric resonator apparatus can be used in the stage coupling with the Qe coupling loop. This results in reduction in the size of the high-frequency band-pass filter apparatus.

Claims: A dielectric resonator apparatus comprising: an electrically conductive case (1); a cross-shaped TM dual mode dielectric resonator (2) provided in said case (1), said TM dual mode dielectric resonator (2) comprising first and second dielectric resonators (3a, 3b) integrally formed so as to be perpendicular to each other; and mode coupling means (4) for coupling an operation mode of said first dielectric resonator (3a) with an operation mode of said second dielectric resonator (3b), formed in said TM dual mode dielectric resonator (2); characterized in that sizes of said first and second dielectric resonators (3a, 3b) are set to be different from each other. The dielectric resonator as claimed in claim 1, wherein said sizes are cross-sectional areas of said first and second dielectric resonators (3a, 3b). The dielectric resonator apparatus, as claimed in claim 1, wherein said sizes are thicknesses of said first and second dielectric resonators (3a, 3b). The dielectric resonator apparatus, as claimed in claim 1, wherein said sizes are widths of said first and second dielectric resonators (3a, 3b). A dielectric resonator apparatus comprising: an electrically conductive case (101) a cross-shaped TM dual mode dielectric resonator (102) provided in said case, said TM dual mode dielectric resonator (102) comprising first and second dielectric resonator (103a,103b) integrally formed so as to be perpendicular to each other; and mode coupling means (104) for coupling an operation mode of said first dielectric resonator (103a) with an operation mode of said second dielectric resonator (103b), formed in said TM dual mode dielectric resonator (102); characterized by a hole (105) for adjusting a resonance frequency of one of said first and second dielectric resonators (103a,103b), formed at an end of one of said first and second dielectric resonators (103a,103b) so as to penetrate the end thereof. A high-frequency band-pass filter apparatus (210) comprising: a first dielectric resonator apparatus (200-1) as claimed in any of claims 1 to 4; a second dielectric resonator apparatus (200-2) as claimed in any of claims 1 to 4; first and second coupling loops (13a,13b) provided in a case (11) so that said first coupling loop (13a) is magnetically connected to said second dielectric resonator (3b) of said first dielectrical resonator apparatus (200-1) and said second coupling loop (13b) is magnetically connected to said second dielectric resonator (3b) of said second dielectric resonator apparatus (200-2); and a partition plate (15) of a metal material having a plurality of slits (14) formed therein so as to be parallel to said second dielectric resonators (3b) of said first and second dielectric resonator apparatus (200-1, 200-2), said slits (14) being provided for magnetically coupling said first dielectric resonator (3a) of said first dielectric resonator apparatus (200-1) with said first dielectric resonator (3a) of said second dielectric resonator apparatus (200-2); wherein due to the different sizes of said first and second dielectric resonators (3a,3b) the resonance frequencies of said second dielectric resonators (3b) of said first and second dielectric resonator apparatus (200-1, 200-2) are equal to those of said first dielectric resonators (3a) thereof. A high-frequency band-pass filter apparatus (211) comprising: A first dielectric resonator apparatus (201-1) as claimed in claim 5; a second dielectric resonator apparatus (201-2) as claimed in claim 5; first and second coupling loops (113a,113b) provided in a case (111) so that said first coupling loop (113a) is magnetically connected to said first dielectric resonator (103a) of said first dielectric resonator apparatus (201-1) and said second coupling loop (113b) is magnetically connected to said first dielectric resonator (103a) of said second dielectric resonator apparatus (201-2); and a partition plate (115) of a metal material having a plurality of slits (114) formed therein so as to be parallel to said first dielectric resonators (103a) of said first and second dielectric resonator apparatus (201-1, 201-2), said slits (114) being provided for magnetically coupling said second dielectric resonator (103b) of said first dielectric resonator apparatus (201-1) with said second dielectric resonator (103b) of said second dielectric resonator apparatus (201-2); wherein a size of said hole (105) is adjusted so that resonance frequencies of said second dielectric resonators (103b) of said first and second dielectric resonator apparatus (200-1, 200-2) are equal to those of said first dielectric resonators (103a) thereof.

Inventors: ABE SHIN, KURISU TORU, WADA HIDEKAZU, ABE, SHIN, KURISU, TORU, WADA, HIDEKAZU
Applicants: MURATA MANUFACTURING CO, MURATA MANUFACTURING CO., LTD.
Application year: 1994
Main classification: H01P1
IPC codes: H01P7, H01P1